Temperature and Heat — Question 9

Section 18-6 · Physics pages 2928–2929

Question 9 A cooling law turns temperature history into transferred heat A body of constant heat capacity C = 600 J/K cools in a 290 K bath. Its measured temperature is T(t) = 290 + 30e−t/120 K, with time in seconds. There is no work and dQ = C dT, positive inward. t T −Tb Axes and labels specify the model; the sketch is schematic. (a) Find the instantaneous signed heat-transfer rate and total heat transferred during the first 120 s. (b) Find the time by which 90% of the total eventual outward heat has left the body.
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Question 9 - Solution A cooling law turns temperature history into transferred heat t T −Tb (a) Method and calculation ˙Q = C dT dt = −150e−t/120 W. Q0→120 = 600[30e−1 −30] ≈−11378.17 J. (b) Interpretation and further calculation Qout,∞= 600(30) = 18000 J. Qout(t) 18000 = 1 −e−t/120 = .90 ⇒t = 120 ln 10 ≈276.31 s. The remaining temperature excess is then 3.00 K. Physical check Outward transfer has negative signed heat; its rate tends to zero as the temperature difference vanishes.

Question 9

A cooling law turns temperature history into transferred heat

A body of constant heat capacity C=600J/KC=600\,\mathrm{J/K} cools in a 290 K bath. Its measured temperature is T(t)=290+30e−t/120T(t)=290+30e^{-t/120} K, with time in seconds. There is no work and dQ=CdTdQ=C\,dT, positive inward.

Diagram shown in the original SVG worksheet.

  1. Find the instantaneous signed heat-transfer rate and total heat transferred during the first 120 s.

  2. Find the time by which 90% of the total eventual outward heat has left the body.

Question 9 - Solution

A cooling law turns temperature history into transferred heat

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Q̇=CdTdt=−150e−t/120W.\dot Q=C\frac{dT}{dt}=-150e^{-t/120}\,\mathrm W.Q0→120=600[30e−1−30]≈−11378.17J.Q_{0\to120}=600[30e^{-1}-30]\approx-11378.17\,\mathrm J.

(b) Interpretation and further calculation

Qout,∞=600(30)=18000J.Q_{\mathrm{out,\infty}}=600(30)=18000\,\mathrm J.Qout(t)18000=1−e−t/120=.90⇒t=120ln⁡10≈276.31s.\frac{Q_{\mathrm{out}}(t)}{18000}=1-e^{-t/120}=.90\ \Rightarrow\ t=120\ln10\approx276.31\,\mathrm s.The remaining temperature excess is then 3.00 K.

Physical check

Outward transfer has negative signed heat; its rate tends to zero as the temperature difference vanishes.